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Some results for the Jacobi-Dunkl transform in the space $L^{2}(\mathbb{R},A_{\alpha,\beta}(t)dt)$

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Some results for the Jacobi-Dunkl transform in the space

L

2

(

R

,

A

α,β

(t)dt)

S. EL OUADIH

a,∗

, R. DAHER

b

and A. BELKHADIR

c

a,b,cDepartement of Mathematics, Faculty of Sciences A¨ın Chock,University Hassan II, Casablanca, Morocco.

Abstract

In this paper, using a generalized Jacobi-Dunkl translation operator, we prove an analog of Titchmarsh’s theorem for functions satisfying the Jacobi-Dunkl Lipschitz condition in L2(R,Aα,β(t)dt),αβ ≥ −21,α6=

−1

2 .

Keywords: Jacobi-Dunkl operator, Jacobi-Dunkl transform, generalized Jacobi-Dunkl translation.

2010 MSC:42B37. c2012 MJM. All rights reserved.

1

Introduction

Titchmarsh’s [[10], Theorem 85] characterized the set of functions in L2(R)satisfying the Cauchy-Lipschitz condition by means of an asymptotic estimate growth of the norm of their Fourier transform, namely we have: Theorem 1.1. [10] Letα∈(0, 1)and assume that f ∈L2(R). Then the following statements are equivalents:

(a) kf(t+h)−f(t)k=0(hα), as h0,

(b)

Z

|λ|≥r

|fb(λ)|2dλ=O(r−2α), as r→∞,

where bf stands for the Fourier transform of f .

In this paper, we prove in analog of Theorem 1.1 for the Jacobi-Dunkl transform for functions satisfying the Jacobi-Dunkl Lipschitz condition in the space L2(R,Aα,β(t)dt). For this purpose, we use the generalized translation operator. Similar results have been established in the context of non compact rank one Riemannian symetric spaces [9].

In section 2 below, we recapitulate from [[1],[2],[3],[5]] some results related to the harmonic analysis associated with Jacobi-Dunkl operatorΛα,β. Section 3 is devoted to the main result after defining the classLip(δ, 2,α,β)

of functions in L2α,β(R) satisfying the Lipschitz condition correspondent to the generalized Jacobi-Dunkl translation.

2

Notation and Preliminaries

The Jacobi-Dunkl function with parameters(α,β),αβ≥ −21,α6= −21, is defined by the formula:

∀x∈R,ψα,βλ (x) =   

 

ϕα,βµ (x)−λi dxd ϕα,βµ (x) ifλC\{0},

1 ifλ=0,

withλ2=µ2+ρ2,ρ=α+β+1 andϕα,βµ is the Jacobi function given by:

ϕα,βµ (x) =F

ρ+iµ

2 ,

ρ−iµ

2 ,α+1,−(sinhx) 2,

Corresponding author.

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where F is the Gausse hypergeometric function (see [1],[6] and [7]).

ψα,βλ is the uniqueC∞-solution onRof the differentiel-difference equation 

Λα,βU =iλU, λC,

U(0) =1, whereΛα,βis the Jacobi-Dunkl operator given by:

Λα,βU(x) = d U(x)

dx + [(2α+1)cothx+ (2β+1)tanhx]×

U(x)− U(−x)

2 ].

The operatorΛα,βis a particular case of the operatorDgiven by

DU(x) = dU(x)

dx + A0(x)

A(x) ×

U(

x)− U(−x) 2

,

where A(x) = |x|2α+1B(x), and B a function of class Con R, even and positive. The operator Λ α,β corresponds to the function

A(x) =Aα,β(x) =2ρ(sinh|x|)2α+1(cosh|x|)2β+1. Using the relation

d dxϕ

α,β

µ (x) =−

µ2+ρ2

4(α+1)sinh(2x)ϕ

α+1,β+1 µ (x), the functionψλα,βcan be written in the form below (see [2])

ψα,βλ (x) =ϕα,βµ (x) +i λ

4(α+1)sinh(2x)ϕ

α+1,β+1

µ (x), x ∈R, whereλ2=µ2+ρ2, ρ=α+β+1.

DenoteL2α,β(R) =L2α,β(R,Aα,β(t)dt)the space of measurable functions f onRsuch that

kfkL2

α,β(R)

=

Z

R|f(t)|

2A α,β(t)dt

1/2

<+∞.

Using the eigenfunctionsψα,βλ of the operatorΛα,βcalled the Jacobi-Dunkl kernels, we define the Jacobi-Dunkl transform of a functionf ∈L2

α,β(R)by: Fα,βf(λ) =

Z

R f(t)ψ

α,β

λ (t)Aα,β(t)dt, λR, and the inversion formula

f(t) =

Z

RFα,βf(λ)ψ

α,β

λ(t)dσ(λ), where

dσ(λ) = |λ|

8πpλ2−ρ2|Cα,β(

p

λ2−ρ2)|

IR\]−ρ,ρ[(λ)dλ.

Here,

Cα,β(µ) = 2

ρ−iµΓ(α+1)Γ(iµ) Γ(1

2(ρ+iµ))Γ(12(αβ+1+iµ))

, µC\(iN),

andIR\]−ρ,ρ[is the characteristic function ofR\]−ρ,ρ[.

DenoteL2

σ(R) =L2(R,dσ(λ)).

The Jacobi-Dunkl transform is a unitary isomorphism fromL2α,β(R)ontoL2σ(R), i.e., kfk:=kfkL2

α,β(R)

=kFα,β(f)kL2

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The operator of Jacobi-Dunkl translation is defined by: Txf(y) =

Z

R f(z)dν

α,β

x,y(z), ∀x,y∈R, (2.2)

whereνα,βx,y(z), x,y∈R, are the signed measures given by

dνα,βx,y(z) =

   

  

Kα,β(x,y,z)Aα,β(z)dz ifx,y∈R∗,

δx ify=0,

δy ifx =0,

here,δxis the Dirac measure atx. And,

Kα,β(x,y,z) = Mα,β(sinh(|x|)sinh(|y|)sinh(|z|))−2αIIx,y×

Z π

0 ρθ(x,y,z) × (gθ(x,y,z))

αβ−1

+ sin2βθdθ,

Ix,y = [−|x| − |y|,−||x| − |y||]∪[||x| − |y||,|x|+|y|],

ρθ(x,y,z) = 1−σxθ,y,z+σzθ,x,y+σzθ,y,x,

∀z∈R,θ∈[0,π],σxθ,y,z=   

 

coshx+coshy−coshzcosθ

sinhxsinhy , ifxy6=0,

0, ifxy=0,

gθ(x,y,z) =1−cosh

2xcosh2ycosh2z+2 coshxcoshycoshzcos

θ,

t+ =

 

t, ift>0, 0, ift≤0, and,

Mα,β =

  

 

2−2ρΓ(α+1)

πΓ(αβ)Γ(β+12) ifα>β,

0 ifα=β.

In [2], we have

Fα,β(Thf)(λ) =ψλα,β(h)Fα,β(f)(λ), λ,h∈R. (2.3)

Forα≥ −21, we introduce the Bessel normalized function of the first kind defined by:

jα(z) =Γ(α+1)

n=0

(−1)n(z2)2n

n!Γ(n+α+1), z∈C.

Moreover, we see that

lim

z→0

jα(z)−1

z2 6=0, by consequence, there existsC1>0 andη>0 satisfying

|z| ≤η⇒ |jα(z)−1| ≥C1|z|2. (2.4) Lemma 2.1. The following inequalities are valids for Jacobi functionsϕα,βµ (t):

(c) |ϕα,βµ (t)| ≤1,

(d) |1−ϕα,βµ (t)| ≤t2(µ2+ρ2). Proof.(See [8], Lemma 3.1, Lemma 3.2).

Lemma 2.2. Letαβ≥ −21,α6= −21. Then for|ν| ≤ρ, there exists a positive constant C2such that |1−ϕα,βµ+iν(t)| ≥C2|1−jα(µt)|.

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3

Main results

In this section we introduce and prove an analog of Theorem 1.1. Firstly we have to define, for functions in L2α,β(R), the conditions of Cauchy-Lipschitz related to the Jacobi-Dunkl translation operator given in 2.2. Definition 3.1. Letδ∈ (0, 1). A function f ∈ L2α,β(R)is said to be in the Jacobi-Dunkl-Lipschitz class, denoted by

Lip(δ, 2,α,β), if

kNhΛmα,βfk=O(hδ), as h→0,

where Nh=Th+T−h−2I, I is the unit operator in the space L2α,β(R)and m=0, 1, 2, .... Lemma 3.3. For f ∈ L2α,β(R), then

kNhΛmα,βfk2=4

Z

Rλ

2m|

ϕα,βµ (h)−1|2|Fα,βf(λ)|2dσ(λ). Proof.SinceFα,βα,βf)(λ) =iλFα,β(f)(λ), we have

Fα,β(Λmα,βf)(λ) =imλmFα,β(f)(λ), m=0, 1, 2, .... (3.5)

We us formulas 2.3 and 3.5, we conclude that Fα,β(NhΛmα,βf)(λ) =im(ψ

α,β λ (h) +ψ

α,β

λ (−h)−2)λ

mF

α,β(f)(λ).

Since

ψα,βλ (h) =ϕα,βµ (h) +i

λ

4(α+1)sinh(2h)ϕ

α+1,β+1 µ (h),

ψα,βλ (−h) =ϕα,βµ (−h)−i λ

4(α+1)sinh(2h)ϕ

α+1,β+1 µ (−h), andϕα,βµ is even (see [2]), then

Fα,β(NhΛmα,βf)(λ) =2im(ϕ α,β

µ (h)−1)λ

mF

α,β(f)(λ).

Now by Parseval’s identity (formula 2.1), we have the result.

Theorem 3.1. Let f ∈ L2α,β(R). Then the following statements are equivalents: (i) f ∈ Lip(δ, 2,α,β),

(ii)

Z

|λ|≥r

λ2m|Fα,β(f)(λ)|2dσ(λ) =O(r−2δ), as r→∞. Proof.(i)⇒(ii). Assume that f ∈ Lip(δ, 2,α,β), then we have

kNhΛmα,βfk=O(hδ), as h→0. From Lemma 3.3, we have

kNhΛmα,βfk2=4

Z

Rλ

2m|1

ϕα,βµ (h)| 2|F

α,β(f)(λ)|2dσ(λ).

By 2.4 and Lemma 2.2, we get:

Z

η

2h≤|λ|≤ η h

λ2m|1−ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ)≥C12C22

Z

η

2h≤|λ|≤ η h

|µh|4|λ2mFα,β(f)(λ)|2dσ(λ).

From 2ηh ≤ |λ| ≤ ηhwe have

η

2h

2

ρ2≤µ2≤ η

h

2

ρ2

µ2h2≥ η

2 4 −ρ

(5)

Takeh≤ η

3ρ, then we haveµ2h2≥C3=C3(η).

So,

Z

η

2h≤|λ|≤ η h

λ2m|1−ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ)≥C12C22C23

Z

η

2h≤|λ|≤ η h

λ2m|Fα,β(f)(λ)|2dσ(λ).

There exists then a positive constantCsuch that

Z

η

2h≤|λ|≤ η h

λ2m|Fα,β(f)(λ)|2dσ(λ)≤C

Z

Rλ

2m|1

ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ)≤Ch2δ.

For all 0<h< η

3ρ, then we have

Z

r≤|λ|≤2r

λ2m|Fα,β(f)(λ)|2dσ(λ)≤Cr−2δ, r→∞.

Furthermore, we obtain

Z

|λ|≥r

λ2m|Fα,β(f)(λ)|2dσ(λ) =

i=0

Z

2ir≤|λ|≤2i+1rλ 2m|F

α,β(f)(λ)|2dσ(λ)

≤ C

i=0

(2ir)−2δ ≤ Cr−2δ. This proves that

Z

|λ|≥r

λ2m|Fα,β(f)(λ)|2dσ(λ) =O(r−2δ), as r→∞.

(ii)⇒(i). Suppose now that

Z

|λ|≥rλ

2m|F

α,β(f)(λ)|2dσ(λ) =O(r−2δ), as r→∞,

and write

Z

Rλ

2m|1

ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ) =

Z

|λ|<1h

λ2m|1−ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ)

+

Z

|λ|≥1h

λ2m|1−ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ).

Using the inequality (c) of Lemma 2.1, we get

Z

|λ|≥1h

λ2m|1−ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ)≤4

Z

|λ|≥1h

λ2m|Fα,β(f)(λ)|2dσ(λ).

Then

Z

|λ|≥1h

λ2m|1−ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ) =O(h2δ), as h→0. (3.6)

Set

φ(λ) =

Z ∞

λ

x2m|Fα,β(f)(x)|2d

σ(x).

An integration by parts gives:

Z x

0 λ 2

λ2m|Fα,β(f)(λ)|2dσ(λ) =

Z x

0 −λ 2

φ0(λ)dλ

= −x2φ(x) +2

Z x

0 λφ(λ)dλ ≤ 2

Z x

0 O

(λ1−2δ)dλ

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From Lemma 2.1, we get

Z

|λ|≤1h

λ2m|1−ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ) ≤

Z

|λ|≤1h

λ2m|1−ϕα,βµ (h)||Fα,β(f)(λ)|2dσ(λ)

Z

|λ|≤1h

λ2m(µ2+ρ2)h2|Fα,β(f)(λ)|2dσ(λ)

≤ h2

Z

|λ|≤1h

λ2λ2m|Fα,β(f)(λ)|2dσ(λ)

= O(h2h−2+2δ). Hence,

Z

|λ|≤1h

λ2m|1−ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ) =O(h2δ). (3.7)

Finally, we conclude from 3.6 and 3.7 that

Z

Rλ

2m|1

ϕα,βµ (h)|2|Fα,β(f)(λ)|2dσ(λ) =

Z

|λ|<1h +

Z

|λ|≥1h = O(h2δ) +O(h2δ) = O(h2δ).

And this ends the proof.

Corollary 3.1. Let f ∈L2α,β(R), and let

kNhΛmα,βfk=O(hδ), as h→0,

Then Z

|λ|≥r

|Fα,β(f)(λ)|2dσ(λ) =O(r−2m−2δ), as r→∞.

4

Acknowledgment

The authors would like to thank the referee for his valuable comments and suggestions.

References

[1] H. Ben Mohamed and H. Mejjaoli, Distributional Jacobi-Dunkl transform and applications, Afr. Diaspora J.Math., 1(2004), 24-46.

[2] H. Ben Mohamed, The Jacobi-Dunkl transform on R and the convolution product on new space of distributions, Ramanujan J., 21(2010), 145-171.

[3] N. Ben Salem and A. Ahmed Salem, Convolution structure associated with the Jacobi-Dunkl operator on

R, Ramanuy J., 12(3)(2006), 359-378.

[4] W. O. Bray and M. A. Pinsky, Growth properties of Fourier transforms via module of continuity, Journal of Functional Analysis., 255(288), 2256-2285.

[5] F. Chouchane, M. Mili and K. Trimche, Positivity of the intertwining operator and harmonic analysis associated with the Jacobi-Dunkl operator onR, J.Anal. Appl., 1(4)(2003), 387-412.

[6] T. H. Koornwinder, Jacobi functions and analysis on noncompact semi-simple Lie groups. in: R. A. Askey, T. H. Koornwinder and W. Schempp(eds) Special Functions: Group theatrical aspects and applications. D. Reidel, Dordrecht (1984).

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[8] S. S. Platonov, Approximation of functions inL2-metric on noncompact rank 1 symmetric space. Algebra Analiz., 11(1)(1999), 244-270.

[9] S. S. Platonov, The Fourier transform of function satisfying the Lipshitz condition on rank 1 symetric spaces, Siberian Math. J., 46(2)(2005), 1108-1118.

[10] E. C. Titchmarsh, Introduction to the theory of Fourier integrals, Claredon , oxford, 1948; Komkniga, Moxow, 2005.

Received: June 09, 2015;Accepted: September 21, 2015

UNIVERSITY PRESS

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